We adopt a boundary integral method to study the dynamics of a translating
droplet confined in a Hele-Shaw cell in the Stokes regime. The droplet is
driven by the motion of the ambient fluid with the same viscosity. We
characterize the three-dimensional (3D) nature of the droplet interface and of
the flow field. The interface develops an arc-shaped ridge near the rear-half
rim with a protrusion in the rear and a laterally symmetric pair of higher
peaks; this pair of protrusions has been identified by recent experiments
(Huerre et al., Phys. Rev. Lett., vol. 115 (6), 2015, 064501) and predicted
asymptotically (Burgess and Foster, Phys. Fluids A, vol. 2 (7), 1990, pp.
1105-1117). The mean film thickness is well predicted by the extended
Bretherton model (Klaseboer et al., Phys. Fluids, vol. 26 (3), 2014, 032107)
with fitting parameters. The flow in the streamwise wall-normal middle plane is
featured with recirculating zones, which are partitioned by stagnation points
closely resembling those of a two-dimensional droplet in a channel.
Recirculation is absent in the wall-parallel, unconfined planes, in sharp
contrast to the interior flow inside a moving droplet in free space. The
preferred orientation of the recirculation results from the anisotropic
confinement of the Hele-Shaw cell. On these planes, we identify a dipolar
disturbance flow field induced by the travelling droplet and its 1/r2
spatial decay is confirmed numerically. We pinpoint counter-rotating streamwise
vortex structures near the lateral interface of the droplet, further
highlighting the complex 3D flow pattern